EP1311813B9 - Systeme et procede pour microscopie de diffusion raman anti-stokes coherente a retrodetection - Google Patents

Systeme et procede pour microscopie de diffusion raman anti-stokes coherente a retrodetection Download PDF

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Publication number
EP1311813B9
EP1311813B9 EP01957072A EP01957072A EP1311813B9 EP 1311813 B9 EP1311813 B9 EP 1311813B9 EP 01957072 A EP01957072 A EP 01957072A EP 01957072 A EP01957072 A EP 01957072A EP 1311813 B9 EP1311813 B9 EP 1311813B9
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Prior art keywords
stokes
pump
cars
detector
sample
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EP1311813A1 (fr
EP1311813A4 (fr
EP1311813B1 (fr
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Xiaoliang Sunney Xie
Andreas Volkmer
Ji-Xin Cheng
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Harvard College
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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
    • G01N21/65—Raman scattering
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28—Investigating the spectrum
    • G01J3/44—Raman spectrometry; Scattering spectrometry ; Fluorescence spectrometry
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00—Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
    • G01N15/10—Investigating individual particles
    • G01N15/14—Optical investigation techniques, e.g. flow cytometry
    • G01N15/1429—Signal processing
    • G01N15/1433—Signal processing using image recognition
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00—Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
    • G01N15/10—Investigating individual particles
    • G01N15/14—Optical investigation techniques, e.g. flow cytometry
    • G01N15/1434—Optical arrangements
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00—Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
    • G01N15/10—Investigating individual particles
    • G01N2015/1006—Investigating individual particles for cytology
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
    • G01N21/65—Raman scattering
    • G01N2021/653—Coherent methods [CARS]

Definitions

  • the invention relates to the field of microscopy, and particularly relates to the field of coherent anti-stokes Raman scattering microscopy.
  • Coherent anti-stokes Raman scattering (CARS) microscopy provides for the imaging of chemical and biological samples by using molecular vibrations as a contrast mechanism.
  • CARS microscopy uses at least two laser fields, a pump electromagnetic field with a center frequency at ⁇ p and a Stokes electromagnetic field with a center frequency at ⁇ s .
  • the Raman shift of ⁇ p - ⁇ s is tuned to be resonant at a given vibrational mode, an enhanced CARS signal is observed at the anti-Stokes frequency ⁇ AS .
  • CARS microscopy does not require the use of fluorophores (which may undergo photobleaching), since the imaging relies on vibrational contrast of biological and chemical materials. Further, the coherent nature of CARS microscopy offers significantly higher sensitivity than spontaneous Raman microscopy. This permits the use of lower average excitation powers (which is tolerable for biological samples). The fact that ⁇ AS > ⁇ p , ⁇ s allows the signal to be detected in the presence of background fluorescence.
  • U.S. Patent No. 4,405,237 discloses a coherent anti-Stokes Raman spectroscopic imaging device in which two laser pulse trains of different wavelengths, temporally and spatially overlapped, are used to simultaneously illuminate a sample.
  • the signal beam in the phase matching direction with a two-dimensional detector, which gives the spatial resolution.
  • U.S. Patent No. 6,108,081 discloses a different method and apparatus for microscopic vibrational imaging using coherent anti-Stokes Raman scattering.
  • collinear pump and Stokes beams were focused by a high numerical aperture (NA) objective lens.
  • NA numerical aperture
  • the nonlinear dependence of the signal on the excitation intensity ensures a small probe volume of the foci, allowing three-dimensional sectioning across a thick sample.
  • the signal beam is detected in the forward direction.
  • FIG. 1 A prior art CARS imaging system (based on the '081 patent) 10 is shown diagrammatically in Figure 1 , in which collinear pump and Stokes beams 12 at frequencies of ⁇ p and ⁇ s respectively, are directed to a microscope objective lens 16, and onto a sample 18.
  • the CARS signal is detected in the forward direction, and is received by collecting optics 20, filtered by one or more filters 22, and detected by a detector 26.
  • the signal beam that is created in CARS imaging includes a substantial amount of background with no vibrational contrast from which the signal must be filtered or somehow distinguished.
  • a conventional (forward-detected) lateral CARS intensity profile of a 535 nm polystyrene bead embedded in water includes a substantial amount of CARS background from water 30 in addition to the characteristic CARS signal from the bead 32.
  • the horizontal axis in Figure 2 represents the lateral dimension (in ⁇ m) across the scan area, and the vertical axis represents the strength of the CARS signal (in cts).
  • the presence of this background from the isotropic bulk water has hindered efforts to increase the sensitivity of CARS imaging, particularly in biological applications.
  • the CARS background is caused by a variety of circumstances. For example, because of electronic contributions to the third order nonlinear susceptibility, there exists a non-resonant contribution to the CARS signal of the sample of interest as well as of the surrounding isotropic bulk medium (i.e., solvent), which is independent of the Raman shift, surrounding isotropic bulk medium (i.e., solvent), which is independent of the Raman shift, ⁇ P - ⁇ S .
  • solvent surrounding isotropic bulk medium
  • a combined CARS image 40 and intensity profile 42 taken along line 44 - 44 of epithelial cells shows that the signal includes CARS background (as generally indicated at 46) that may not be easily distinguished from the microscopic sample signal (as generally indicated at 48).
  • the lateral dimension (in ⁇ m) is shown along the horizontal axis, and signal strength (in cts) is shown along the vertical axis. In certain embodiments, these bulk solvent background contributions to the detected CARS signal may overwhelm the CARS sample signals.
  • the system includes at least two laser sources, a pump source for generating an electromagnetic field at the pump frequency, a Stokes source for generating an electromagnetic field at the Stokes frequency that is different from the pump frequency, optics to direct collinearly the pump and Stokes beams toward an objective lens, which provides a common focal spot, and a detector for measuring a coherent anti-Stokes signal in the backward (epi) direction that is generated by the interaction of pump and Stokes fields with the sample, and collected by the same lens focusing the pump and Stokes beams.
  • a pump source for generating an electromagnetic field at the pump frequency
  • a Stokes source for generating an electromagnetic field at the Stokes frequency that is different from the pump frequency
  • optics to direct collinearly the pump and Stokes beams toward an objective lens, which provides a common focal spot
  • a detector for measuring a coherent anti-Stokes signal in the backward (epi) direction that is generated by the interaction of pump and Stokes fields with the sample, and collected by the same lens focusing the
  • the radiation field of CARS emits in both the forward direction and in the backward direction with respect to the direction of incident pump and Stokes fields on the sample 56 as shown at 58 in Figure 4 .
  • the backward directed portion 54a of the coherent radiation field equals the forward directed portion 52a, resembling the radiation field pattern of a Hertzian dipole.
  • a system in accordance with an embodiment of the invention includes collimated and collinear pump and Stokes fields 60.
  • the fields are generated by lasers at a pump frequency ( ⁇ P ) and a Stokes frequency ( ⁇ S ), and in further embodiments three fields may be used.
  • Both fields 60 are directed to a high numerical aperture (NA) objective lens 66 by a dichroic beamsplitter 64, and lens 66 focuses both fields 60 to a common spot into the sample 70.
  • NA numerical aperture
  • the same lens 66 collects the backward (or epi) directed radiation field, which is then transmitted through the dichroic beamsplitter 64.
  • the latter together with additional filters 74 spectrally isolates the CARS radiation before being detected.
  • An epi-detected CARS signal is thereby received at the detector 78.
  • one or more lenses may be used to focus the epi-detected signal onto the detector 78.
  • Conventional optical image scanning schemes e.g. three-dimensional sample stage scanning or incident beam scanning
  • the detector 78 permit the sample to be thereby imaged.
  • the underlying principle of the E-CARS microscope system of Figure 5 may be qualitatively described by considering the physical picture in which the pump and Stokes fields are assumed to be monochromatic plane waves that propagate along the z axis as indicated at 80 in Figure 6 through a slab sample having a thickness of D .
  • P (3) is the third-order polarization
  • c is the vacuum velocity of light
  • n AS is the refractive index at the anti-Stokes angular frequency, ⁇ AS .
  • the phase matching condition is
  • D ⁇ 0 the phase matching condition is satisfied in both the forward direction ( k AS along the z direction) and backward direction (k AS along the -z direction). This provides that the forward and backward CARS signals are equal in intensity for a thin sample.
  • D increases, however, the forward signal begins to overwhelm the backward signal because of the constructive interference in the forward direction and the destructive interference in the backward direction.
  • the forward CARS signal (
  • 0) has a quadratic dependence on D, I AS F ( D ) ⁇ D 2 . Contribution to the signal from the solvent (large D ) may, therefore, overwhelm the contribution from a thin sample (small D ).
  • the signal oscillates as a function of D with a periodicity of ⁇ AS /2 n , I AS E ( D ) ⁇ ⁇ AS 2 sin 2 (2 ⁇ nD / ⁇ AS ).
  • the contribution from the solvent (large D ) is significantly reduced as compared to that of the forward CARS signal.
  • the above analysis involved the assumption that the pump and Stokes signals are plane waves. Although these signals are actually tightly focused beams in the present embodiment, the physical picture described above remains the same.
  • the forward and backward CARS signals for tightly focused beams may [the] quantitatively analyzed by assuming that the incident pump and Stokes fields propagate along the optical axis z, and that they are linearly polarized along the x axis as indicated at 82.
  • the field distribution is no longer Gaussian because of the breakdown of the paraxial approximation.
  • the y and z components of the fields near the focal point are relatively small and can be neglected.
  • ⁇ x 2 + y 2
  • J 0 is the zero-order Bessel function.
  • a spherical sample 84 with a diameter D is placed at the origin of the overlapped foci of the pump and Stokes fields. Again assuming that any differences between the refractive indexes of the sample and solvent are negligible, the incident fields may be assumed to be unperturbed by the presence of the sample.
  • the forward detected CARS signal 90 increases quasi-quadratically with D and becomes saturated when D exceeds the longitudinal dimension of the focal excitation volume, i.e., full width at half maximum (FWHM) ⁇ 1.2 ⁇ m for the experimental condition.
  • FWHM full width at half maximum
  • the epi-detected CARS signal appears only for small spheres and exhibits several maxima with the highest one art ⁇ 0.65 ⁇ P , and a periodicity close to that under the plane wave condition ( ⁇ AS /2 n ).
  • the epi-detected CARS signal intensity is negligible for spheres of large D, which resembles the case of focusing into an isotropic bulk medium.
  • the ratio 94 of the intensities of the epi-detected CARS signal to the forward detected CARS signal establishes the presence of epi-detected CARS signals for small scatterers under the tightly focused condition.
  • the numerical aperture of the lens was 1.4, and the index of refraction of the medium was 1.52.
  • the refractive index mismatch between the sample and the solvent which is not considered in the calculation, can cause back-reflection of forward-going CARS (F-CARS).
  • F-CARS forward-going CARS
  • the back-reflected F-CARS is defocused, and can be minimized by using confocal detection. If the size of the scatterer is small, the back-reflected F-CARS signal from the scatterer is negligible. For larger scatterers, however, the back - reflected CARS signal might be used as an additional contrast mechanism in epi-detection.
  • a CARS system that combined the elements of Figures 1 and 5 was developed for recording both the forward detected CARS signal and the epi-detected CARS signal simultaneously.
  • a regeneratively amplified Ti:sapphire laser system that pumped an optical parametric amplifier (RegA 9000/OPA 9400, coherent) and operated at a repetition rate of 250 kHz was used to provide femtosecond pulses (FWHM ⁇ 110 fs) for the excitation fields.
  • Both linearly polarized pump and Stokes beams were temporally overlapped by an optical delay line, collinearly sent into an inverted optical microscope (Nikon TE 300 sold by Nikon Instruments, Inc.
  • CARS images were collected by raster scanning the sample with respect to the fixed laser beams using a closed-loop piezo-driven two-dimensional scanning stage.
  • the collinear pump and Stokes beams may be raster scanned with respect to the fixed sample.
  • the lateral profile of the forward detected CARS intensity is shown in Figure 2
  • the lateral profile of the simultaneously recorded epi-detected CARS signal is shown at 100 in Figure 8 .
  • the CARS signals were confirmed by the quadratic and linear dependence on the incident pump and Stokes intensities, respectively.
  • FIG. 2 A comparison of Figures 2 and 8 illustrates the efficient rejection of isotropic bulk solvent contributions to the detected signal and the increase in sensitivity of the epi-detected CARS microscopy.
  • the signal-to-background ratio for forward detected CARS was about 1.5, whereas that for epi-detected CARS was greater than 20. It has been found that the epi-detected CARS of pure water is more than a factor of 100 smaller than the simultaneously measured forward detected CARS, which is consistent with the illustration in Figure 8 .
  • a polystyrene bead having a diameter of 1 ⁇ m was imaged by an epi-detected CARS microscope system. Similar results to those discussed above were obtained. As shown in Figure 9A at 110, the intensity of the epi-detected CARS signal exhibits a square-dependence on the pump peak power / kW, and as shown at 120 in Figure 9B , the intensity of the epi-detected CARS signal is linearly dependent on the Stokes peak power / kW.
  • epi-detected CARS imaging of an unstained epithelial cell in an aqueous environment is illustrated in Figure 10 .
  • the incident pump and Stokes fields were at 13333.2 cm -1 and 11762.8 cm -1 respectively, and the Raman shift was 1570 cm -1 , which is within the region of signature Raman bands of proteins and nucleic acids.
  • the image size was about 512 x 512 (pixel) 2 with an integration time of 4.88 ms per pixel.
  • the combined epi-detected CARS image 130 and lateral intensity profile 132 taken along line 134 - 134 illustrates the efficient rejection of the aqueous solvent signal (as generally indicated at 136), as well as the identification of small diffraction-limited features with high signal-to-background ratios (as generally indicated at 138).
  • the nucleus, and other intracellular components are clearly observed with the epi-detection, which otherwise could not be seen with the forward-detected CARS as was the case with the image shown in Figure 3 .
  • the image contrast disappears when the pump and Stokes pulses are not temporally or spatially overlapped.
  • epi-detected CARS microscopy may significantly increase the sensitivity of CARS detection for scatterers that are smaller than the wavelength of light. This technique is particularly suited for intracellular imaging, although the invention may be employed in a wide variety of other applications where a small signal of a microscopic CARS scatterer has to be extracted from a relatively large CARS background originating from an isotropic bulk medium. It should be noted that the same concept of engineering the phase-matching condition by employing the epi-detection scheme is generally applicable to other nonlinear coherent microscopy schemes, such as but not limited to second harmonic generation, sum frequency generation and third harmonic generation. Epi-detected CARS may also be readily implemented with conventional confocal epi-fluorescence microscopes and provides improved sensitivity for point-by-point chemical mapping of living cells with vibrational spectroscopy.

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Claims (15)

  1. Système destiné à détecter un signal de diffusion Raman anti-Stokes cohérent induit dans un échantillon microscopique, ledit système comprenant : une source de pompe destinée à générer un champ électromagnétique de pompe à une fréquence de pompe (ωp), une source de Stokes destinée à générer un champ électromagnétique de Stokes à une fréquence de Stokes (ωs) qui est différente de ladite fréquence de pompe (ωp) ; une optique (64) destinée à diriger lesdits champs électromagnétiques de pompe et de Stockes (60) de manière colinéaire par l'intermédiaire d'une lentille de mise au point (66) vers un volume focal commun (70) dans une première direction.
    caractérisé en ce que
    ledit système comprend en outre un filtre (74) et un détecteur (78) destiné à détecter un signal de diffusion Raman anti-Stokes cohérent filtré de manière spectrale, qui est généré dans une deuxième direction par l'interaction des champs électromagnétiques de pompe et de Stokes dans le volume focal (70), ladite deuxième direction étant sensiblement opposée à ladite première direction.
  2. Système selon la revendication 1, dans lequel ledit système comprend en outre une optique de détecteur destinée à diriger le signal de diffusion Raman anti-Stokes cohérent qui est généré dans la deuxième direction vers ledit détecteur (78).
  3. Système selon la revendication 2, dans lequel ledit système comprend en outre un séparateur de faisceaux dichroïque (64) positionné entre ladite lentille de mise au point (66) et ledit détecteur (78).
  4. Système selon la revendication 1, dans lequel ledit champ cohérent non linéaire se déplace à travers un séparateur de faisceaux dichroïque (64) dans son déplacement en direction dudit détecteur (78).
  5. Système selon la revendication 1, dans lequel ledit système comprend en outre un échantillon qui est soumis à un balayage récurrent par rapport aux faisceaux fixes.
  6. Système selon la revendication 1, dans lequel ledit système comprend en outre des faisceaux qui sont soumis à un balayage récurrent par rapport à un échantillon fixe (70).
  7. Système selon la revendication 1, dans lequel ledit signal de diffusion Raman anti-Stokes cohérent est reçu par le détecteur (78) après un retour par l'intermédiaire de l'optique qui a dirigé les champs électromagnétiques de pompe et de Stokes (60) vers le volume focal commun (70).
  8. Système selon la revendication 8, dans lequel ledit champ cohérent non linéaire est reçu par le détecteur (78) après un retour par l'intermédiaire de la lentille de mise au point (66) qui a dirigé les premier et deuxième champs électromagnétiques vers le volume focal commun (70).
  9. Système selon l'une quelconque des revendications précédentes, dans lequel ledit détecteur (78) destiné à détecter le champ cohérent non linéaire mesure le signal anti-Stokes cohérent dans la deuxième direction.
  10. Procédé de détection d'un signal de diffusion Raman anti-Stokes cohérent induit dans un échantillon microscopique, ledit procédé comprenant les étapes consistant à : générer un champ électromagnétique de pompe à une fréquence de pompe (ωp), générer un champ électromagnétique de Stokes à une fréquence de Stokes (ωs) qui est différente de ladite fréquence de pompe ; diriger lesdits champs électromagnétiques de pompe et de Stokes (60) de manière colinéaire par l'intermédiaire d'une lentille de mise au point (66) vers un volume focal commun (70) dans une première direction ;
    caractérisé en ce que
    le procédé comprend en outre un filtrage et une détection du signal de diffusion Raman anti-Stokes cohérent filtré de manière spectrale qui est généré dans une deuxième direction par l'interaction des champs électromagnétiques de pompe et de Stokes dans le volume focal (70), ladite deuxième direction étant sensiblement opposée à ladite première direction.
  11. Procédé selon la revendication 10, où ledit procédé comprend en outre l'étape consistant à diriger le signal de diffusion Raman anti-Stokes cohérent du volume focal (70) en retour par l'intermédiaire de ladite lentille de mise au point (66).
  12. Système selon la revendication 1, dans lequel la lentille de mise au point (66) est un objectif à ouverture numérique élevée.
  13. Système selon la revendication 1, dans lequel le détecteur (78) est une photodiode à avalanche (APD).
  14. Système selon la revendication 1, dans lequel le système comprend deux lasers Ti: saphir picosecondes pompés de manière synchrone.
  15. Système selon la revendication 1, dans lequel le système comprend de plus un détecteur de direction vers l'avant destiné à détecter un champ anti-Stokes cohérent qui est généré à partir du volume focal dans une direction vers l'avant.
EP01957072A 2000-07-13 2001-06-20 Systeme et procede pour microscopie de diffusion raman anti-stokes coherente a retrodetection Expired - Lifetime EP1311813B9 (fr)

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US20030160955A1 (en) 2003-08-28
EP1311813A1 (fr) 2003-05-21
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US6809814B2 (en) 2004-10-26
EP1311813B1 (fr) 2012-01-25
WO2002006778A1 (fr) 2002-01-24

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